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(1)

R ENDICONTI

del

S EMINARIO M ATEMATICO

della

U NIVERSITÀ DI P ADOVA

J. C HABROWSKI

Dirichlet problem for a linear elliptic equation in unbounded domains with L

2

-boundary data

Rendiconti del Seminario Matematico della Università di Padova, tome 71 (1984), p. 287-328

<http://www.numdam.org/item?id=RSMUP_1984__71__287_0>

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(2)

Elliptic Equation

in Unbounded Domains with L2 - Boundary Data.

J. CHABROWSKI

1. Introduction.

The main purposes of this paper are to

investigate

the Dirichlet

problem

for the

elliptic equation

in a

half-space

and a

complement

of a bounded open set. We shall refer to the second

problem

as the exterior Dirichlet

problem.

Given an open set Q c we denote

by

the Banach space of functions u in

Z2(S~) having

weak

(distributional)

derivatives

Diu.

(i = 1, ..., n)

in

L2(Q).

A norm is introduced

by defining

The closure of in

Wl,2(Q)

is denoted

by

A local space consists of functions

belonging

to for every bounded open set ,~’ such that S~.

To motivate our

approach

to the Dirichlet

problem

assume for

simplicity

that .~ is

uniformly elliptic

and the coefficients c

(*)

Indirizzo dell’A.:

Department

of Mathematics,

University

of Queens- land, St. Lucia Queensland 4067, Australia.

(3)

and

f

are measurable and bounded on SZ. A function u is said to be

a weak solution of the

equation (1)

if u E and u satisfies

for every v

EWl,2(Q)

with

compact support

in ,~. Let q E

_L2(aS2)

and assume that there is a function ffJl E

Wl,2(Q)

such that q = ffJ1

on a,~ in the sense of trace. A weak solution in of the equa- tion

(1)

is a solution of the Dirichlet

problem

with the

boundary

condi-

tion u = 99 on 8Q if The basic results

concerning

the Dirichlet

problem

in W1,2-framework can be found in

Ladyzhens- kaja

and Ural’ceva

[16], Gilbarg

and

Trudinger [10]

and

Stampacchia [24], [25].

In the above definition it is assumed that the

boundary data

is a trace of some function

belonging

to

Wl,2(Q).

This condi- tion is rather

restrictive,

because not every function in

L 2

is the

trace of some function

belonging

to

(see

Lions and

Mage-

nes

[17]

Theorems 7.5 and 9.4

Chapter 1).

It is clear that the Dirichlet

problem

with

L2-boundary

data

requires

a new definition. The first

attempt

to define the Dirichlet

problem

with

L2 -boundary

data has

been made

by

Mikhailov who in a series of articles

[11], [18], [19]

and

[20]

examined this

problem

in a bounded domain under the assump- tion aij E

CI(D) and bi,

c E

(see

also Necas

[22]

and

[23]).

Similar

results were also obtained

by Kapanadze [15].

The author and

Thomp-

son

[5]

extended Mikhailov’s results to the

equation

with coefficients

satisfying

some

general integrability

conditions. In the articles men- tioned above the

boundary

8Q

belongs

to C2. For the

Laplace equation

the Dirichlet

problem

with

L2-boundary

data was solved in bounded

Lipschitz

domains

(see Dahlberg [8],

Jerrison and

Kenig [12], [13]).

We mention here that Jerrison and

Kenig

also extended their results to bounded non-smooth domains for an

equation

with C’-eoefficients

(see [14]).

The

plan

of this paper is as follows. In sections 1-6 we examine the Dirichlet

problem

in a half space. The main result is an energy estimate

(section 3,

the

inequality (19))

for the

equation

~u

+

lu =

f,

where I is a

sufficiently large parameter.

Next

applying

the result

of Bottaro and Marina

[3]

we establish the existence of a

unique

solu-

tion to the Dirichlet

problem

with

L2-boundary

data for the

equation (1)

with the condition

e(x) ~

Const &#x3E; 0. In sections

7,

8 and 9 similar

results are established for the exterior Dirichlet

problem.

Methods

(4)

used in both cases are similar and

presented

in some details. We

point

out that the

assumptions

on the coefficients ai~ for the Dirichlet

problem

in the half space are

considerably

weaker than the

correspond- ing assumptions

for the exterior Dirichlet

problem.

This follows from

the fact that the

boundary

of the half space is flat.

Among

the papers devoted to

study

the

boundary

value

problems

in unbounded domains

we mention the work of Benci and Fortunato

[2],

in which the Dirichlet

problem

with zero

boundary

data in a

weighted

Sobolev space has been studied.

In this paper we make

frequent

use of the Sobolev

inequality

where

The most

significant

feature of this

inequality

lies in the

independence

of the constant S of the domain S~ which makes

possible

to use it in

unbounded domains

(see

Federer

[9]).

2. Traces.

Let

Rt

= &#x3E;

01.

We denote a

point

x E

Ri by x

=

= (x’,xn),

where x’= ... , I

Throughout

sections 2-6 we make the

following assumptions

about

the

operator

L :

(A)

.L is

uniformly elliptic

in

.Rn , i.e.,

there exists a

positive constant y

such that

for all

and $ e Rn ,

moreover

(i, j = 1, ..., n).

(B) (i)

There exist

positive

constants x and 0 a 1 such that

for all and all

oo) .

(5)

All constants in this paper will be denoted

by C~ .

The statement

«

C, depends

on the structure of the

operator

1)&#x3E; means that

Ci depends

on n, a,

b, k,

m, and the norms of the coefficients

Daij,

ai;,

bi

and

c in

appropriate

spaces. co

In the

sequel

we shall need the

following elementary

lemmas.

is bounded

independently of 6

E

(0, T/2].

PROOF.

Integrating by parts

Denoting

the last

integral by

J and

applying Young’s inequality

(6)

we obtain

Taking s

=

(1

-

y)/4

the result follows.

We also need the

following simple

observation.

LEMMA 3. let be a solution

of (1 ).

Then

for

every

where a

positive

constant C

depends

on the structure

of

the

operator

Land r.

PROOF. Let v =

U02

where 0 E

Using

v as a test function in

( 2 )

we obtain

It follows from

ellipticity

of L and the

inequalities

of

Young

and

Sobolev that

where a

positive

constant C

depends

on the structure of the

operator

JD. Here we have used the fact that c = c1

+

C2 with Cl E J~ and c, E

To

complete

the

proof put 0 = 0, ,

where

0,

is an

increasing

sequence

(7)

of

non-negative

functions in with the

gradient

bounded inde-

pendently

of v and

converging

as v --~ oo to a

non-negative

function

f on

lit equal

to 1 for and

vanishing

for

THEOREM 1. be a solution

of (1)

in

~.

Then the

following

conditions are

equivalent :

PROOF. Let

0 C 38o C 1.

Define a

non-negative

function

q e C2 ([0, oo))

such that = xn for and

21(x,,)

= 1 for

We may assume that

q(rn) &#x3E; 6

for all and 0

6 60.

Let

where 0 is a

non-negative

function in Since for

every 6

C x~

v( ~, xn)

has a

compact support

in it follows from Lemma 5 that

v is an admissible test function in

(2),

hence

Denote the

integrals

on the left hand side of

(4) by J1,

...,

Je.

It follows

(8)

from the

ellipticity

of .~ that

By Young’s inequality

where a

positive

constant

01 depends

on y and

Similarly

where a

positive

constant

C, depends

on

11 bi ll,..

Now

according

to

the

assumption (B iii)

where °1 E and 02 E

By

Hölder’s

inequality

where

1/2*

=

1 /2 - 11n.

Now

by

Sobolev’s

inequality

(9)

were 8

depends only

on n. Since we may assume

we obtain

by Young’s inequality

where a

positive

constant

03 depends

on n, and y.

By

Green’s formula we have

and

by

the

assumption (B ii)

where a

positive

constant

C,~ depends

on and xi .

Integrating

by parts

(10)

By

the

assumption (Bi)

we obtain

where a

positive

constant

C, depends

on x, y and From the last

inequality

we deduce the

following

estimate for

J.,

where a

positive

constant

06 depends

on x, and

. Inserting

the estimates

(5)-(10)

into

(4)

we obtain

(11)

If the condition

(I)

holds then

by

Lemma 1 the

integrals

are bounded

independently

of 6. Now

put 0 = 0,, where 0,

is an

increasing

sequence of

non-negative

functions in

tending

to

1 as v - oo with the

gradient

bounded

independently

of v.

Letting

v - oo in

(11)

it follows from Lemma 3 that

The

implication

o I ~ II » follows from Lemmas 1 and 3 and the

Lebesgue

convergence theorem.

To show that « II =&#x3E; I » observe that

(12)

Now

by

Lemma 2 the condition

(II) implies

that the

integrals

are bounded

independently

of 6.

Repeating

the

argument

from the

step

«I =&#x3E;Tl)) the result follows.

REMARK 1. It follows from the

proof

Theorem 1 that the condi- tion

(II) implies:

As an immediate consequence we obtain , COROLLARY 1..Let u E be a solution

o f (1)

in

that one

of

the conditions

(I)

or

(II)

holds. Then there exists a

function

q E and a sequence

6,

- 0 as v - oo such that

for

every

THEOREM be a solution

o f (1)

in

R:. Suppose

that one

of

th e conditions

( I )

or

( II )

holds. Then there exists a

function

~ E such that

for every Y E L2(Rn-1).

PROOF. Since

~)2

dx’ is

bounded,

say and

ann(x’, 6)

~n-l

continuous and bounded it follows from

Corollary 1,

that

(13)

It suffices to show the existence of the

and

v(x)

= 0

elsewhere, where 77 oo))

is

the

function introduced in the

proof

of Theorem 1.

Taking v

as a test function in

(2)

we obtain

Since for every 0

y

1

"ri "n

and Y has a

compact support,

the

Lebesgue

dominated convergence theorem

implies

the

continuity

of

Now

By

the

Lebesgue

dominated convergence theorem and the

previous

(14)

part

of the

proof,

the

right

hand side of the last

inequality

tends to

0 as b - 0 and this

completes

the

proof.

Our next

objective

is to establish the

L2-convergence

of

u( ~, ð)

to 99 as 6 - 0. To do this we first show that the norm of

u( ., ð)

converges to the norm of 99. The result then follows

by

the uniform

convexity

of the space

L2.j

THEOREM 3. Let U E

IVI,2 (R,+,)

be a solution

of (1 ). Suppose

that

one

of

the conditions

(I)

or

(II)

holds. Then there exists a

function

99 E L2

(Rn_1)

such that

PROOF. If Il E

1’1’ ~’Z~lLn~~

then

by

the

argument

used in the

proof

of Theorem 1 we obtain

where q

is the function introduced in the

proof

of Theorem 1. Define

(15)

it is clear that . Thus

We shall show that

.and

(15)

Indeed

(16)

Here we have used the fact that u is a solution of

(1)

and the

identity (2)

with the test function

where 27

is the function introduced in the

proof ’of

Theorem 1.

To prove

(15)

observe that

.

Using

the conditions

(I), (II)

and Lemma 1 one can show that We

only

restrict ourselves to the term

J,.

(17)

Integrating by parts

the term

J3

can be written in the

following

form

Hence

by

the

assumption (B ii)

where a

positive

constant C

depends

on xl, n and

(~== 11

...I

n -1). By

Lemma 1 the first

integral

on the

right

hand side tends to 0 as 6 -~ 0. Now

by

H61der’s

inequality

It

follows

from the condition

(I)

that

and

consequently by

the condition

(II)

the second

integral

on the

right

hand side of

(16)

also tends to 0 as 6 - 0. It follows from

(~.3),

(18)

(14)

and

(15)

that

To

complete

the

proof

observe that the norms

are

equivalent

in

3.

Energy

estimate.

Consider the

elliptic equation

of the form

in where A is a real

parameter.

The results of section 2

suggest

the

following

definitian of the Dirichlet

problem.

A weak solution

is a solution of the Dirichlet

problem

with the

boundary

condition

The main result of this section is the

following

energy estimate.

THEOREM 4. Let I be a solution

of

the Dirichlet

problems

(17), (18).

Then there exist

positive

constants

d, Ao

and C

independent

of

’11, such that

(19)

for all

A&#x3E;

where a

positive

constant C

depends

on the structure of L.

PROOF. Since is a solution of the Dirichlet

problem

for certain

30

&#x3E; 0 and

consequently by

Theorem 1 the condition

(II)

holds. All constants

appearing

in

the

proof

are

indepenent

of 8 and

depend

on the structure of L and may vary from line to line.

By

the same considerations as in the

proof

of the

step

I =&#x3E; II » of Theorem 1 we show that

~o, whereq

is the function introduced in the

proof

of Theorem 1.

Letting 6

- 0 we deduce from the last

inequality

It

follows

from

(20)

and

(3) (see

Lemma

3)

that

(20)

Now

adding

the

inequalities (3)

and

(21)

we

get

By

a similar manner

(see

the

proof

of the

step

« I =&#x3E; II » of Theorem

1)

we obtain

Now

inserting (22)

into

(23)

we obtain

(21)

Now we make use of the

following

fact: for every

0 ~ ~O

1 and 0

d

1

Thus

(19)

follows from

(22)

and

(23) provided A

is

sufficiently large

and d

sufficiently

small.

. Dirichlet

problem

in

Ri.

We are now in a

position

to establish the existence of a solution

to the Dirichlet

problem.

THEOREM

~, ~ ~,o

Assume that r1

(i =1,

..., n)

and that Then

for (Rn_i )

there

exists a

unique

solution

of

the Dirichlet

problem (17), (18)

in

PROOF. Let

(qm)

be a sequence of functions in

converging

in

L2(Rn_i)

to the function 99. Put

~rn =

1, 2, ....

. It follows from

[3]

that there exists a

unique

solution

in

&#x3E;

of the Dirichlet

problem

(22)

By

Theorem 4

for where C is a

positive

constant

independent

of p and q. Con-

sequently

is the

Cauchy

sequence in the norm

and the result follows.

THEOREM 6.

Suppose

that the

essumptions of

Theorem 5 hold and

moreover 0 Then

for

there

exists a

unique

solution to the Dirichlet

problem (1), (18)

in

and moreover

where C is a

positive

constant

depending

on the structure

of

the

operator

L.

PROOF. Let

lo

be a

sufficiently large positive

constant.

By

Theorem

5 the Dirichlet

problem

has a

unique

solution in

loc n satisfying

the energy estimate

(25).

On the other hand in virtue of Theorem 1.1 in

[3]

the Dirichlet

problem

(23)

has a

unique

solution in

~W1~2(.Rn )

and moreover

where C is a

positive

constant. Thus the function u = ~o

-f- v

is a solution of the

problem (1), (18)

and it is obvious that

where C is a

positive

constant. To obtain the estimate

(25)

it suffices

to derive the estimate of the form

(23)

for sup

~)2

dx’ and then

Rn_1

use the final

part

of the

argument

of the

proof

of Theorem 4 and the

inequality (27).

The next result establishes the relation between the solution of the Dirichlet

problem

in and

T~1’2(.Rn).

We

point

out here

that

by

a solution of the Dirichlet

problem

in we mean a

solution of

(1)

with the

boundary

condition in the sense of trace

(see Introduction).

THEOREM 7.

Suppose

that the

assumptions of

Theorem 6

hold,

that

and that there exists a

f unction

such that

q;l(X’, 0 )

_

~p(x’ )

on

Rn-l in

the sense

o f

trace. Then the solution

o f

the

Dirichlet

problem (1), (18)

in solution

of

the same

problem

in

PROOF. It follows from

[3]

that the Dirichlet

problem

Zu =

f

on

.Rn

and u = y on

Rn-l

has a solution in which is also a

solution in The result follows from the

uniqueness

of the

solutions in of the

problem (1), (18).

5.

Weighted

estimate of the

gradient.

It is well known that a solution of the Dirichlet

problem

for the

Laplace equation

(24)

where q;

EL2(Rn-t)

satisfies the

following

relation

-"n

The

question

arises whether the

inequality,

RTn

remains true for the solution of the

problem (1), (18)

in

c (see [26]

p.

82-83).

The

following

theorem contains

a

partial

answer to this

question.

THEOREM 8.

Suppose

that

c(x) &#x3E; Const

&#x3E; 0 orc 7 c E

+ + bi

= 0

(i

=

1,

...,

n)

and

f

= 0 on

X -

Let u be a solution

of

the Dirichlet

problem (1), (18)

in Then

where a

positive

constant C

depends

on the structure

of

the

operator

L.

PROOF. Let be an

increasing

sequence of functions in

C2([o, oo))

converging

to rn on

[0, c&#x3E;o)

with

properties: i7,(x,,)

= xn for

q(rn) &#x3E; 3

for xn &#x3E;

2 60

and

~D2~v ~

are bounded

indepen- dently

of v. q, may be chosen to be constant for

large

Xnè i,

Taking

as a test function in

(2)

we obtain

We denote the sum of the second and third

integral by J1

and

integrat-

(25)

ing by parts

we obtain

where a

positive

constant

C, depends

on m.,, sup

ID*17,1

and

sup

ID2,7,1. Similarly

the fourth

integral Jg

can be estimated in the

following

way

where a

positive

constant

O2 depends

on "1’ and

supID77,1.

+

Finally using

the

ellipticity

and the fact that c is bounded below

by

.a

positive

constant we obtain

etting

v - oo and 6 - 0 we derive from the last

inequality

(26)

where

positive

constants

C3

and

Õ3 depend

on the structure of the opera- tor .~. Now

applying

the energy estimate

(25)

we obtain

(28).

REMARK 2. The estimate

(28)

can be extended to the nonhomo-

I

geneous

equation provided

1

6. Estimate of derivatives of’ the second order.

In this section we

replace

the

assumptions (B i)

and

(B ii) by

the

following

condition

( k, i, j,

=

1,...,’n),

where

b and x1 are positive

constants.

THEoRF,3i 9. u be a solution in

loc of

the

problem (1), (18).

T hen

where C is a

positive

constant

depending

on the structure

o f

L.

PROOF. It follows from Theorem 8.8 in

[10] (p.173) that u

E

We shall first show that for every r &#x3E; 0

Indeed, taking v

=

Dkw,

where w E with

compact support,

as a test function in

(2)

and

integrating by parts

we obtain

(27)

Now let w = where 0 is a

non-negative

function in such that W = 0 for and

xERn-l.

Then

Applying

the

inequalities

of

H61der, Young

and Sobolev we deduce from the last

equation

that

where a

positive

constant C

depends

on the structure of L. Now

put

where

(Py

is an

increasing

sequence of

non-negative

functions

in with

supports

in on

and with bounded

independently

of v.

Letting

v - 00 the ine-

quality (30)

follows. To establish

(29)

let

where 77

is a function introduced in the

proof

of Theorem 1.

By (30)

(28)

~,u is an admissible test function in

(31)

and

We may assume

Applying

the

inequalities

of

Young,

Holder and Sobolev we

easily

derive from the last

inequality

the follow-

ing

estimate

(29)

where C is a

positive

constant

depending

on the structure of the opera- tor

L,

and the result follows.

7.

Exterior Dirichlet problem.

Preliminaries.

Let Q c

Rn

be a

complement

of a bounded closed set with

boundary

8Q of class C2. we consider the

equation (1).

Let x E

Q,

we denote

by r(x)

the distance from x to 3D.

We make the

following assumptions

There exists a

positive

constant y such that

for all x E .~

and ~

moreover aij E

L’(92)

r1

(i, j

=

1,

...,

n).

We also assume that

xr(x)-a (i, j

=

1,

... ,

n)

in some

neigh-

bourhood N of the

boundary 8Q,

where x &#x3E; 0 and 0 a 1 are cons- tants and that

Dkaii N) (k, i, j

=

1,

...,

n).

(~2) bi

E

f

E

22(Q)

and c E

+ Ln(,Q) (i

=

1,

...,

n).

It follows from the

regularity

of the

boundary

8Q that there is

a number

~o &#x3E; 0

such that the domain

with

boundary

possesses the

following property:

to each

ro e 8Q

there is a

unique point ro(so)

= xo - where

v(xo)

is the outward normal to 8Q at xo .

According

to Lemma 1 in

[10]

p.

382,

the distance

r(x) belongs

to

C2(Q -

if

6,

is

sufficiently

small. We extend

r(x)

as

positive

function of class

C2(Q)

and

denote this extension

again by r(x).

We may assume that N c Q -

Do..

Let xa denote an

arbitrary point

of

8Qd.

For fixed 6 E

(0,

let

and

(30)

where

IA I

denote the

(n - 1)-dimensional

Hausdorff measure of

A,

and

vo(xo)

is the outward normal to at xo. Mikhailov

[19] proved

that there is a

positive

number Yo such that

We will use the surface

integral

where u E and the values of

son

are understood in the sense of trace.

Let

Ro

be a

positive

number such that

Qo

c

.R~

for

every R &#x3E;

Ro .

Set

°

for all

..R &#x3E; .Ro .

In the

sequel

we shall need the

following

estimate: if

and p

is a constant in

[0,1),

then

for 6 E

(0, ðo/4],

where .~1 is a

positive

constant

independent

of 6 and u.

This

inequality

can be established

by

the same

argument

as in the

proof

of Lemma

2;

in the

proof

we use the

inequality (32).

Moreover it is easy to see that if

M(6)

is bounded on

(0, ~o]

then

for every p E

[0,1)

(31)

for all 6 E

(0, bo/21,

where

M1

is a

positive

constant

independent

of

~ and u.

THEOREM 10. Let u be a solution

of (1 ) belonging

to

Wlo~(SZ).

Then

the

following

conditions are

equivalent

PROOF. We

only

sketch the

proof

because it is identical to that of Theorem 1 in

[5].

Fix an .R &#x3E; and let 0 be a

non-negative

func-

tion in such that = 1 for

lxl c.R

and

Ø(x)

= 0 for

Ixl

&#x3E; 2R.

Suppose

that holds. Thus u E

)

for

every

&#x3E;

.Ro

and

(34)

holds. It is clear that

is an admissible test function in

(2)

and

By

Green’s formula

(see [21],

p.

139)

we have

(32)

and

By

the

ellipticity

condition and the

inequalities

of

Young

and Sobolev

we derive from

(35), (36)

and

(37)

that

Now choose q _

0,,

where

(Wr)

is an

increasing

sequence of non-

negative

functions in

converging

to 1 for with

IDØ,I

bounded

independently

of v.

Letting 6 - o

and v - oo the result

easily

follows.

Now suppose that the condition

(Ill)

holds.

By (35)

and

(36)

we have

Using (33)

and the

inequalities

of

Young,

Holder and

Sobolev,

it

is easy to see that

M(6)

is bounded on

(0, 5o].

Our next

objective

is to prove that u has a trace on aS~ in

L2(ôQ).

We first state the

following preliminary result,

which is easy to prove

(see

Theorems 2 and 3 of Section

2).

THEOREM 11..Let be a solution

of (1). Assume

that

one

of

the conditions

(Ii)

or

(III)

holds. Then there exists a

function

(33)

such that

for

every g E

_L2(aQ).

To prove that - 99 in

L2(ôQ)

we show that

and the result follows from the uniform

convexity

of

~SE

_ _

Fix .R &#x3E;

.Ro,

E

(0, ~o]

we define the

mapping lJ2R

-~

by

where

xa(x)

denotes the nearest

point

to x on and =

xa~2(x)

for each x E 3D. Moreover &#x3E;

5/2

and x8 is

uniformly Lipschitz

continuous. Note that if u E then

u(r’)

E for each

..R &#x3E;

Ro .

To prove

L2-convergence

of we shall need the

following

tech-

nical lemmas

LEMMA 4.

I f rif

and then

5.

If gEL2(QR)

and

r!fEL2(QR)

and suppose that

is bounded on

(0, ~o],

then a.,

with inner

product (norm)

denoted

with inner

product (norm)

denoted

(34)

THEOREM 12. Let u E

loc

be a solution

of (1 )

such that one

of

the conditions

(11)

or holds. Then there is a

function

99 c such that

u(xa)

converges to 99 E

PROOF. The

proof

is similar to that of Theorem 4 and is the

repeti-

tion of the

argument given

in the case of bounded domain

(Theorem

4

in

[~]) .

Since

B1.BB1

and

11.112

are

equivalent

it sufficient to show that there

is 99

E

L:

2 such that lim

u(xi)

= 99 in 2

By

uniform

convexity

of

.~2

it suffices to show that

By

Green’s theorem we find that

Let 0 be defined as in the

proof

of Theorem

10,

then

Consequently

we obtain

for 6 E

(0, 30],

since = x on

,SZa,2R

and = 1 on

DR.

We show

that

(35)

and

since = on

aS2.

The relation

(38)

follows from Lemmas 4 and 5. To establish

(39)

we use

(2)

with a test function v

given by

the

following

formula

Theorem

12 justifies

the

following

definition of the Dirichlet

problem.

A weak solution of

(1)

is a solution

of the Dirichlet

problem

with the

boundary

condition

B.

Energy

estimate for the exterior Dirichlet

problem.

Assume that the distance function

r(x)

is extended into S~ in such

a way that

on &#x3E;

Ro),

where

1~1

is a

positive

constant.

Let q~

E and consider the

following

Dirichlet

problem

in

(36)

where A is a real

parameter.

If

A&#x3E; 10 (10 sufficiently large)

then

by

Theorem 6 in

[5]

there exists a

unique

solution. The

boundary

condi-

tions

(44)

is understood in the sense of

L2-convergence and by (43)

we mean that

Wlt2(QR)

for every function P E such that P =1 in some

neighbourhood

of

Ix

_ Rand P = 0 on Q -

LEMMA 6.

Suppose

that r

satisfies

the condition

(E)

and let u be a

solutions in

loc ) of

the Dirichlet

problem (42), (43)

and

(44).

Then

there exist

10

&#x3E; 0

(sufficiently large)

and d &#x3E; 0

(sufficiently small)

such

that

for

all

R &#x3E; .Ro,

where

positive

constant

Âo,

d and C

depend

on the struc-

ture

of

the

operator

and acre

independent o f

R.

PROOF. The energy estimate

(45)

was

essentially proved

in

[5].

We

repeat

the

proof

to show that the constants

0,

d and

Ao

are

indepen-

dent of R. Let

on

elsewhere .

By

Green’s theorem

(37)

Now

applying Holder

y

Young

and Sobolev

inequalities

we obtain

-where a

positive

constant

Ci

is

independent

of .Z~. On the other hand

we have

Letting 8 -

0 in

(47)

we obtain

It follows from

(48)

and

(49)

that

-where

O2

and

03

are

positive

constants

independent

of .R. Now observe that

by

the

assumption (E)

we have

(38)

where and

where and

consequently

Similarly

Choosing

d

sufficiently

small and

Ao sufficiently large

the result follows from

(48), (49), (50), (51)

and

(52).

9. Existence of a solution of the exterior Dirichlet

problem.

It is clear that one can deduce from Lemma 6 the existence of a solution of the Dirichlet

problem (42), (43)

and

(44)

in

-Wl,2

As an immediate consequence of Lemma 6 we obtain

THEOREM 13.

Suppose

that the distance

f unction

r

satisfies

the condi-

tion

(E) . Let

99 E and

f (x)2r(x)

dx oo. Then

for

every

À;;;. Ào

there exists ac

unique

solution

of

the Dirichlet

problem (42), (40)

and

(41)

in and moreover

where a

positive

constant 0

depends

on the structure

of

the

operator

L.

(39)

PROOF. For fixed .R &#x3E;

.Ro

consider a

solution vR

of the

problem (42), (43)

and

(44)

and set

vR(x)

= 0 for

lxl

&#x3E; .R. It follows from the energy estimate

(45)

that there exists a sequence vR

tending weakly

to

a solution of the

problem (42), (40)

and

(41).

From now on introduce the

following assumption

on the distance

function r

(F)

The distance function

r(x)

on is extended to a function in

C2(,~)

such that

r(x)

= 1 on S~ n

~ .Ro~.

It is obvious that condition

(F) implies (E).

THEOREM 14. In addition to the

hypotheses

and

(A2)

assume

that

bi

E

(i

=

1,

...,

n),

c E

+

and c &#x3E; Const. &#x3E; 0

on Q. let and Then there exists a

unique

solu-

tion u

of

the Dirichlet

problem (1 ), (40)

and

(41)

in and moreover

where a

positive

constant C

depends

on the structure

o f

Z.

The

proof

is similar to that of Theorem 6 and therefore is omitted.

We

only point

out that we

again

use here the results of Bottaro and Marina

[3].

Under our

assumption

a solution in of the

problem (1), (40)-(41) belongs

to

By

the same

argument

as in the

proof

of Theorem 9 one can establish the

following

estimate of the derivative

of the second order of a solution in of the

problem (1), (40)

and

(41).

THEOREM 15.

Suppose

that the

assumptions of

Theorem 14 hold.

Let ’U be a solution in

of

the

problem (1), (40)

and

(41).

Then

where C is a

positive

constant

depending

on the structure

of

the

operator

~.

(40)

We mention here that the estimate of the derivative of the second order of a solution of the exterior Dirichlet

problem

in

~2~2(S~)

was

obtained

by

Acanfora

[1].

10. Case

c ~ 0.

To establish the existence and the

uniqueness

of a solution of the

Dirichlet

problem

we have assumed that c ~ Const &#x3E; 0. If the coeffi- cient c is

only non-negative

one can also construct a solution but

belonging

to a different function space.

Namely

introduce the space

~1,2(Rn ) equipped

with the norm

and

similarly

for the exterior Dirichlet

problem

the space

Jf’1,2(Q)

with the norm

where r s atisfies the condition

(.F’). By

Theorem 7 a solution of the

Dirichlet

problem (1), (18) belongs

and

by

Theorem 14 a

solution of the exterior Dirichlet

problem (1), (40)

and

(41) belongs

to

y~l~ 2(,~)

.

Now denote

by (D(Q))

the

completion

of

with

respect

to the norm

By

Sobolev’s

inequality (D(S2) c ~2*(S~)),

whence

c

(-D(S2)

c

THEOREM 16.

Suppose

that the

assumptions (A)

and

(B )

hold. Let

f

e

.L2 (.I~ ) a’nd lfJ

e and moreover assume that

b

e

(i

=

1, ..., n),

and on Then there exists a sol’U- t’ion ’U to the Dirichlet

problem (1), (18), belonging to the

space

W1,2(R+n) +

+

(41)

Here the

boundary

condition

(18)

is satisfied in the

following

sense:

for

every .R

&#x3E; 0

PROOF. Consider the Dirichlet

problem

where the

boundary

condition is understood inthe sense of L2-conver- gence

(see

section

3).

If

Ao

is

sufficiently large

then

by

Theorem 5

there exists a

unique

solution uo

belonging

to the space

T~1’2(.Rn ).

On the other hand

by

the result of Chicco

[7]

the Dirichlet

problem

has a solution in

D(X).

It is clear that v

+

uo is a solution of

(1), (18)

in

T~’1’2(.Rn ) -~- D(.Rn ). The L2-convergence

in the sense

(54)

follows

from the fact that

In a similar manner one can establish

THEOREM 17.

Suppose

that the

assumptions (A1)

and

(A2)

hold.

.Let 99

E and moreover assume that

bi

E

(i =1,

...,

n),

c E

Ln/2(,Q)

and

c(x) ~

0 on 92. Then there exists a solution

of

the Dirichlet

problem (1), (40)

and

(41)

in

+ D(SZ).

REFERENCES

[1] F. ACANFORA, Problema esterno di Dirichlet per una classe di

equazioni

ellittiche del secondo ordine, Rend. Accad. Sei. Fis. Mat.

Napoli,

65

(1979),

pp. 59-69.

(42)

[2] V. BENCI - D. FORTUNATO, Second order

elliptic

operators on unbounded

domains,

Boll. Un. Mat. Ital., (5), 15 (1978), pp. 193-209.

[3]

G. BOTTARO - M. E. MARINA, Problema di Dirichlet per

equazioni

ellittiche

di

tipo

variazionale su insiemi non limitati, Boll. Un. Mat. Ital., (4), 8 (1973), pp. 46-56.

[4] J. CHABROWSKI - B. THOMPSON, On traces

of

solutions

of a

semi-linear

partial differential equations of elliptic

type, to appear in Ann. Polon.

Math.

[5] J. CHABROWSKI - B. THOMPSON, On the

boundary

values

of

solutions

of

linear

elliptic equations,

Bull. Austral. Math. Soc., 27 (1983), pp. 1-30.

[6] J. CHABROWSKI, Note on

nontangential boundary

limits

of

solutions

of elliptic equations in divergence form,

to appear in

Manuseripta

Math.

[7] M. CHICCO, An

apriori inequality

concerning

elliptic,

second order

partial differential equations of

variational type, Matematiche

(Catania),

26 (1971),

pp. 172-182.

[8] B. E. J. DAHLBERG, On the Poisson

integral for Lipschitz

and C1-domains, Studia Math., 64 (1979), pp. 13-24.

[9] H. FEDERER - W. H. FLEMING, Normal and

integral

currents, Ann. of Math., 72 (1960), pp. 458-520.

[10] D. GILBARG - N. S. TRUDINGER,

Elliptic partial differential equations of

second order,

Springer-Verlag,

Berlin -

Heidelberg -

New York, 1977.

[11] A. K. GUSCIN - V. P. MIKHAILOV, On the

boundary

values in L-

(p &#x3E;

1)

of

solutions

of elliptic equations,

Mat. Sb., 108 (150) (1979), pp. 1-19.

[12]

D. S. JERISON - C. E. KENIG,

Boundary

behaviour

of

harmonic

functions

in

non-tangentially

accessible domains,

preprint,

Department of Mathe- matics, Princeton

University.

[13] D. S. JERISON - C. E. KENIG,

Boundary

value

problems

in

Lipschitz

do- mains,

preprint.

[14] D. S. JERISON - C. E. KENIG, The Dirichlet

problem

in nonsmooth do- mains, Ann. of Math., 13 (1981), pp. 367-382.

[15] J. V. KAPANADZE, On

boundary

values

of a

second order linear

elliptic equations,

Bulletin of the

Academy

of Science of the

Georgian

S.S.R., 93 (1979), pp. 285-288.

[16]

O. A. LADYZHENSKAJA - N. N. URAL’TSEVA, Linear and

quasilinear elliptic equations,

Academic Press, New York and London, 1968.

[17] J. LIONS - E. MAGENES, Problèmes aux limites non

homogenes

et

appli-

cations, vol. 1, Dunod, Paris, 1968.

[18] V. P. MIKHAILOV,

Boundary

values

of

solutions

of elliptic equations

in

the ball, Mat. Sb., 100 (142) (1972), pp. 1-13.

[19]

V. P. MIKHAILOV, Dirichlet’s

problem for a

second order

elliptic equation, Differential’nye Uravnenija,

12 (1976), pp. 1877-1891.

[20] V. P. MIKHAILOV, On the

boundary

values

of

the solutions

of elliptic

equa- tions,

Appl.

Mat.

Optim.,

6 (1980), pp. 193-199.

[21] V. P. MIKHAILOV, Partial

differential

equations, Mir Publishers, Moscow, 1978.

(43)

[22] J.

NE010DAS,

On the

regularity of

second order

elliptic partial differential equations

with unbounded Dirichlet

integral,

Arch. Rational Mech.

Anal.,

9 (1962), pp. 134-144.

[23]

J. NECAS, Les methodes directes en théorie des

équations elliptiques,

Aca- demia,

Éditeurs, Prague,

1967.

[24]

G. STAMPACCHIA, Le

problème

de Dirichlet pour les

équations elliptiques

du second ordre à

coefficients

discontinus, Ann. Inst. Fourier

(Grenoble),

15 (1969), pp. 189-258.

[25] G. STAMPACCHIA,

Équations elliptiques

du second ordre à

coefficients

dis-

continus, Les Presses de l’Université de Montréal, Séminaire de Mathé-

tiques Supérieurs

(1965).

[26]

E. STEIN,

Singular integrals

and

differentiability properties of functions,

Princeton

University

Press, Princeton, New

Jersey,

1970.

Manoscritto

pervenuto

in redazione il 18 febbraio 1983.

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